Abstract

Although the passively adjusting and actively tuning of pure longitudinal (primary (P-)) and pure transverse (secondary or shear (S-)) waves band structures in periodically laminated piezoelectric composites have been studied, the actively tuning of coupled elastic waves (such as P-SV, P-SH, SV-SH, and P-SV-SH waves), particularly as the coupling of wave modes is attributed to the material anisotropy, in these phononic crystals remains an untouched topic. This paper presents the analytical matrix method for solving the dispersion characteristics of coupled elastic waves along the thickness direction in periodically multilayered piezoelectric composites consisting of arbitrarily anisotropic materials and applied by four kinds of electrical boundaries. By switching among these four electrical boundaries—the electric-open, the external capacitance, the electric-short, and the external feedback control—and by altering the capacitance/gain coefficient in cases of the external capacitance/feedback-voltage boundaries, the tunability of the band properties of the coupled elastic waves along layering thickness in the concerned phononic multilayered crystals are investigated. First, the state space formalism is introduced to describe the three-dimensional elastodynamics of arbitrarily anisotropic elastic and piezoelectric layers. Second, based on the traveling wave solutions to the state vectors of all constituent layers in the unit cell, the transfer matrix method is used to derive the dispersion equation of characteristic coupled elastic waves in the whole periodically laminated anisotropic piezoelectric composites. Finally, the numerical examples are provided to demonstrate the dispersion properties of the coupled elastic waves, with their dependence on the anisotropy of piezoelectric constituent layers being emphasized. The influences of the electrical boundaries and the electrode thickness on the band structures of various kinds of coupled elastic waves are also studied through numerical examples. One main finding is that the frequencies corresponding to (with the dimensionless characteristic wavenumber) are not always the demarcation between pass-bands and stop-bands for coupled elastic waves, although they are definitely the demarcation for pure P- and S-waves. The other main finding is that the coupled elastic waves are more sensitive to, if they are affected by, the electrical boundaries than the pure P- and S-wave modes, so that higher tunability efficiency should be achieved if coupled elastic waves instead of pure waves are exploited.

Highlights

  • Multilayered composite structures [1,2,3] are constituted by periodically arranged unit cell with multilayered configuration

  • In summary of the above literature review on various types of elastic waves in laminated piezoelectric phononic crystals with both passive and active electrical boundary conditions, we propose the following five insufficiencies that exist in the investigations so far: 1

  • Consider the elastic waves propagating along the thickness direction, i.e., perpendicular to the interface, in infinitely periodically laminated piezoelectric composite structures whose unit cell, as shown in Figure 1, consists of any number of arbitrarily anisotropic piezoelectric and elastic layers with the piezoelectric interlayers having anyone of four electrical boundaries such as the electric-open, the applied electrical capacitance, the electric-short, and the applied feedback control conditions

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Summary

Introduction

Multilayered composite structures [1,2,3] are constituted by periodically arranged unit cell with multilayered configuration. Considering both metallized and non-metallized interfaces, Piliposyan et al [54] analyzed by TMM the dispersion curves and the reflection/transmission of inclined SH-type guided waves in the infinite periodic composites or in the finite counterparts with a defect layer as the mirror symmetry center and two piezoelectric half-spaces on both sides as substrates The dependences of these wave behaviors on the ratio of the unit cell’s length to the waveguide’s height, the piezoelectric material properties, the boundary condition distribution on the lower and upper walls, and the presence of defect layer were discussed, with special attention on the Bragg resonances and the presence of trapped modes and slow waves.

Basic Model
State Space Formalism
Section 3.1.2.
The State Equation of a Piezoelectric Layer
The Traveling Wave Solution to the State Equation of a Layer
Transfer Matrix Method
Transfer Relation of an Elastic Layer
Transfer Relation of a Piezoelectric Layer
Transfer Relation of an Interface
Transfer Relation of the Unit Cell
Numerical Examples
Dispersion Properties of Coupled Elastic Waves
11. The influence of electrode thicknesson onthe the band of the and coupled
Conclusions
Reference
2014, 040802, Methods
Full Text
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